Near- and Far-Field Characterization of Stationary Plasma Thruster Plumes

A comprehensive investigation of Hall thruster plume plasma ion energy distribution functions and ion charge state has been made on both e ight- and laboratory-model engines. An energy analyzer, mass spectrometer, and E £ B probe were used to characterize Hall thruster plume ions. The results of this investigation show that the distribution function of the ion beam exhibits both Maxwellian and Druyvesteyn traits and that the Hall thruster plumecontainsa nontrivial amountofenergetic,multiplycharged particlesthat mustbeaccounted forinmodeling the erosion rate of solar array cover glass and interconnect material. Detection of these multiply charged ions by energy analyzers has been hampered in the past by charge exchange and elastic collisions. The high-energy tail seen in numerous energy analyzer data is thought to result from charge exchange and elastic collisions between singly and multiply charged ions and neutrals. The role of facility pressure was also investigated and was found to have an ine uence mainly on the width of the ion energy distribution function. This pressure broadening is caused by elastic collisions between beam ions and background chamber gas particles. Nomenclature B = magnetic e eld vector, T E = electric e eld, V /m E = electric e eld vector, V /m Eb = ion beam energy, eV Ei = ion energy, eV f = ion distribution function f .Ei/ = ion energy distribution function f .v/ = ion velocity distribution function Ii = E£B probe collector current, A ni = ion number density, m i3 q = elementary charge, C qI = charge state of ion r = position vector, m t = time, s ui = ion speed, m /s Vi = beam ion acceleration potential, V v = ion velocity vector, m /s

[1]  Eric Pencil,et al.  Far-field plume contamination and sputtering of the stationary plasma thruster , 1994 .

[2]  Takao Yoshikawa,et al.  Basic Operational Characteristics and Thrust Performance of Low Power Hall Thrusters. , 2002 .

[3]  James S. Sovey Improved ion containment using a ring-cusp ion thruster , 1984 .

[4]  F. Gulczinski Examination of the structure and evolution of ion energy properties of a 5 kW class laboratory Hall effect thruster at various operational conditions. , 1999 .

[5]  P. Peterson,et al.  An experimental investigation of the internal magnetic field topography of an operating Hall thruster , 2002 .

[6]  J. Pollard,et al.  Plume angular, energy, and mass spectral measurements with the T5 ion engine , 1995 .

[7]  H. R. Kaufman,et al.  Technology of closed-drift thrusters , 1983 .

[8]  John M. Sankovic,et al.  Hall thruster ion beam characterization , 1995 .

[9]  R. Vahrenkamp Measurement of double charged ions in the beam of a 30-cm mercury bombardment thruster , 1973 .

[10]  John N. Anderson,et al.  Fullerene propellant research for electric propulsion , 1996 .

[11]  H. Rundle,et al.  Electron Energy Distribution Functions in an O2 Glow Discharge , 1973 .

[12]  T. W. Haag,et al.  End-hall thrusters , 1990 .

[13]  Michael J. Patterson,et al.  Performance characteristics of ring-cusp thrusters with xenon propellant , 1986 .

[14]  Gregory G. Spanjers,et al.  Performance characteristics of a 5 kW laboratory hall thruster , 1998 .

[15]  Lyon B. King Transport-property and mass spectral measurements in the plasma exhaust plume of a Hall-effect space propulsion system , 1998 .

[16]  C. O. Brown,et al.  Further Experimental Investigations of a Cesium Hall-Current Accelerator , 1964 .

[17]  Alec D. Gallimore,et al.  Gridded retarding pressure sensor for ion and neutral particle analysis in flowing plasmas , 1997 .

[18]  G. R. Seikel,et al.  Basic studies of a low density hall current ion accelerator , 1966 .